Relativistic electromagnetism

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Relativistic electromagnetism is a physical phenomenon explained in electromagnetic field theory due to Coulomb's law and Lorentz transformations.

Electromechanics[edit]

After Maxwell proposed the differential equation model of the electromagnetic field in 1873, the mechanism of action of fields came into question, for instance in the Kelvin’s master class held at Johns Hopkins University in 1884 and commemorated a century later.[1]

The requirement that the equations remain consistent when viewed from various moving observers led to special relativity, a geometric theory of 4-space where intermediation is by light and radiation.[2] The spacetime geometry provided a context for technical description of electric technology, especially generators, motors, and lighting at first. The Coulomb force was generalized to the Lorentz force. For example, with this model transmission lines and power grids were developed and radio frequency communication explored.

An effort to mount a full-fledged electromechanics on a relativistic basis is seen in the work of Leigh Page, from the project outline in 1912[3] to his textbook Electrodynamics (1940)[4] The interplay (according to the differential equations) of electric and magnetic field as viewed over moving observers is examined. What is charge density in electrostatics becomes proper charge density[5][6][7] and generates a magnetic field for a moving observer.

A revival of interest in this method for education and training of electrical and electronics engineers broke out in the 1960s after Richard Feynman’s textbook.[8] Rosser’s book Classical Electromagnetism via Relativity was popular,[9] as was Anthony French’s treatment in his textbook[10] which illustrated diagrammatically the proper charge density. One author proclaimed, "Maxwell — Out of Newton, Coulomb, and Einstein".[11]

The use of retarded potentials to describe electromagnetic fields from source-charges is an expression of relativistic electromagnetism.

Principle[edit]

The question of how an electric field in one inertial frame of reference looks in different reference frames moving with respect to the first is crucial to understanding fields created by moving sources. In the special case, the sources that create the field are at rest with respect to one of the reference frames. Given the electric field in the frame where the sources are at rest, one can ask: what is the electric field in some other frame?[12] Knowing the electric field at some point (in space and time) in the rest frame of the sources, and knowing the relative velocity of the two frames provided all the information needed to calculate the electric field at the same point in the other frame. In other words, the electric field in the other frame does not depend on the particular distribution of the source charges, only on the local value of the electric field in the first frame at that point. Thus, the electric field is a complete representation of the influence of the far-away charges.

Alternatively, introductory treatments of magnetism introduce the Biot–Savart law, which describes the magnetic field associated with an electric current. An observer at rest with respect to a system of static, free charges will see no magnetic field. However, a moving observer looking at the same set of charges does perceive a current, and thus a magnetic field. That is, the magnetic field is simply the electric field, as seen in a moving coordinate system.

See also[edit]

Notes and references[edit]

  1. ^ Kargon, Robert; Achinstein, Peter (1987). Kelvin’s Baltimore Lectures and Modern Theoretical Physics: Historical and philosophical perspectives. MIT Press. ISBN 0-262-11117-9.
  2. ^ What led me more or less directly to the special theory of relativity was the conviction that the electromotive force acting on a body in motion in a magnetic field was nothing else but an electric field. Albert Einstein (1953) Shankland, R. S. (1964). "Michelson-Morley Experiment". American Journal of Physics. 32: 16–81. Bibcode:1964AmJPh..32...16S. doi:10.1119/1.1970063.
  3. ^ Page, Leigh (1912). "Derivation of the Fundamental Relations of Electrodynamics from those of Electrostatics". American Journal of Science. 34: 57–68. Bibcode:1912AmJS...34...57P. doi:10.2475/ajs.s4-34.199.57. If the principle of relativity had been enunciated before the date of Oersted’s discovery, the fundamental relations of electrodynamics could have been predicted on theoretical grounds as a direct consequence of the fundamental laws of electrostatics, extended so as to apply to charges relatively in motion as well as charges relatively at rest.
  4. ^ Page, Leigh; Adams, Norman Ilsley (1940). Electrodynamics. D. Van Nostrand Company.
  5. ^ Mould, Richard A. (2001). Basic Relativity. Springer Science & Business Media. § 62, Lorentz force. ISBN 0387952101.
  6. ^ Lawden, Derek F. (2012). An Introduction to Tensor Calculus: Relativity and Cosmology. Courier Corporation. p. 74. ISBN 0486132145.
  7. ^ Vanderlinde, Jack (2006). Classical Electromagnetic Theory. Springer Science & Business Media. § 11.1, The Four-potential and Coulomb’s Law, page 314. ISBN 1402027001.
  8. ^ Feynman, Richard (1964). The Feynman Lectures on Physics. 2. Section 13-6.
  9. ^ Rosser, W.G.V. (1968). Classical Electromagnetism via Relativity. Plenum Press.
  10. ^ French, Anthony (1968). Special Relativity. W. W. Norton & Company. Chapter 8.
  11. ^ Tessman, Jack R. (1966). "Maxwell - Out of Newton, Coulomb, and Einstein". American Journal of Physics. 34: 1048–1055. Bibcode:1966AmJPh..34.1048T. doi:10.1119/1.1972453.
  12. ^ Purcell, Edward M. (1985) [1965]. Electricity and Magnetism. Berkeley Physics Course. 2 (2nd ed.). McGraw-Hill.